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ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Lec 6: September 19, 2016 MOS Model Penn ESE370 Fall2016 – Khanna You are Here: Transistor Edition ! Previously: simple models (0 and 1st order) " ! This week and next (4 lectures) " " " ! Comfortable with basic functions and circuits Detailed semiconductor discussion MOSFET phenomenology Don’t Blink! Rest of term " Implications of the MOS device Penn ESE370 Fall2016 – Khanna 2 Today ! ! ! MOS Structure Basic Fabrication Semiconductor Physics " " " " " Metals, insulators Silicon lattice Band gaps Doping Field Effects Penn ESE370 Fall2016 – Khanna 3 MOS ! Metal Oxide Semiconductor Penn ESE370 Fall2016 – Khanna 4 MOS ! ! Metal – gate Oxide – insulator separating gate from semiconductor " ! ! Ideally: no conduction from gate to semiconductor Semiconductor – between source and drain See why gate input is capacitive? gate drain source semiconductor Penn ESE370 Fall2016 – Khanna 5 Capacitor ! ! Charge distribution and field? How much charge on plates? gate drain source semiconductor Penn ESE370 Fall2016 – Khanna 6 Idea ! ! ! Semiconductor – can behave as metal or insulator Voltage on gate induces an electrical field Induced field attracts (repels) charge in semiconductor to form a channel " " Semiconductor can be switched between conducting and not conducting Hence “Field-Effect” Transistor gate drain source semiconductor Penn ESE370 Fall2016 – Khanna 7 Source/Drain Contacts ! Contacts: Conductors # metalic " Connect to metal wires that connect transistors Penn ESE370 Fall2016 – Khanna 8 Fabrication ! ! ! ! ! Start with Silicon wafer Dope Grow Oxide (SiO2) Deposit Metal Mask/Etch to define where features go http://www.youtube.com/watch?v=35jWSQXku74 Time Code: 2:00-4:30 Penn ESE370 Fall2016 – Khanna 9 Dimensions ! Channel Length (L) Channel Width (W) Oxide Thickness (Tox) ! Process named by minimum length ! ! " 22nm # L=22nm Penn ESE370 Fall2016 – Khanna 10 Semiconductor Physics Penn ESE370 Fall2016 – Khanna 11 Conduction ! ! ! Metal – conducts Insulator – does not conduct Semiconductor – can act as either Penn ESE370 Fall2016 – Khanna 12 Why does metal conduct? ! (periodic table) http://chemistry.about.com/od/imagesclipartstructures/ig/Science-Pictures/Periodic-Table-of-the-Elements.htm Penn ESE370 Fall2016 – Khanna 13 Why does metal conduct? Penn ESE370 Fall2016 – Khanna 14 http://commons.wikimedia.org/wiki/File:Periodic_Table_of_Elements_showing_Electron_Shells.svg Why does metal conduct? Penn ESE 370 Fall 2016 - Khanna 15 Conduction ! ! Electrons move Must be able to “remove” electron from atom or molecule Penn ESE370 Fall2016 – Khanna 16 Atomic States ! Quantized Energy Levels (bands) " ! Valence and Conduction Bands Must have enough energy to change level (state) Penn ESE370 Fall2016 – Khanna 17 Thermal Energy ! Except at absolute 0 " " There is always free energy Causes electrons to hop around " " ….when there is enough energy to change states Energy gap between states determines energy required Penn ESE370 Fall2016 – Khanna 18 Silicon Atom ! How many valence electrons? Penn ESE370 Fall2016 – Khanna 19 Silicon ! 4 valence electrons " " Inner shells filled Only outer shells contribute to chemical interactions Penn ESE370 Fall2016 – Khanna 20 Silicon-Silicon Bonding ! Can form covalent bonds with 4 other silicon atoms Penn ESE370 Fall2016 – Khanna 21 Silicon Lattice ! Forms into crystal lattice Penn ESE370 Fall2016 – Khanna 22 Silicon Ingot 1 impurity atom per 10 billion silicon atoms Penn ESE370 Fall2016 – Khanna 23 23 Silicon Lattice ! Cartoon two-dimensional view Penn ESE370 Fall2016 – Khanna 24 Outer Orbital? ! What happens to outer shell in Silicon lattice? Penn ESE370 Fall2016 – Khanna 25 Energy? ! What does this say about energy to move electron? Penn ESE370 Fall2016 – Khanna 26 Energy Energy State View Valance Band – all states filled Penn ESE370 Fall2016 – Khanna 27 Energy State View Energy Conduction Band– all states empty Valance Band – all states filled Penn ESE370 Fall2016 – Khanna 28 Energy State View Energy Conduction Band– all states empty Band Gap Valance Band – all states filled Penn ESE370 Fall2016 – Khanna 29 Band Gap and Conduction Insulator Metal Ec 8ev Ec Ev OR Ev Ev Ec Semiconductor 1.1ev Penn ESE370 Fall2016 – Khanna Ec Ev 30 Doping ! Add impurities to Silicon Lattice " Replace a Si atom at a lattice site with another Penn ESE370 Fall2016 – Khanna 31 Doping ! Add impurities to Silicon Lattice " ! Replace a Si atom at a lattice site with another Add a Group 15 element " " E.g. P (Phosphorus) How many valence electrons? Penn ESE370 Fall2016 – Khanna 32 Doping ! Add impurities to Silicon Lattice " ! Replace a Si atom at a lattice site with another Add a Group 15 element " " E.g. P (Phosphorus) How many valence electrons? Penn ESE370 Fall2016 – Khanna 33 Doping with P Penn ESE370 Fall2016 – Khanna 34 Doping with P ! End up with extra electrons " ! Donor electrons Not tightly bound to atom " " Low energy to displace Easy for these electrons to move Penn ESE370 Fall2016 – Khanna 35 Doped Band Gaps ! Addition of donor electrons makes more metallic " Easier to conduct Semiconductor 0.045ev 1.1ev Penn ESE370 Fall2016 – Khanna Ec Ev ED 36 Localized ! Donor electron is localized " ! Won’t go far if no low energy states nearby Increasing doping concentration " " Ratio of P atoms to Si atoms Decreases energy to conduct Penn ESE370 Fall2016 – Khanna 37 Electron Conduction Penn ESE370 Fall2016 – Khanna 38 Electron Conduction Penn ESE370 Fall2016 – Khanna 39 Capacitor Charge ! Remember capacitor charge ++++++++ - - - - - - - - - Penn ESE370 Fall2016 – Khanna gate drain source semiconductor 40 MOS Field? ! What does “capacitor” field do to the Donor-doped semiconductor channel? Vgs=0 No field - - - - - - Penn ESE370 Fall2016 – Khanna 41 MOS Field? ! What does “capacitor” field do to the Donor-doped semiconductor channel? Vgs=0 No field + - - - - - - Penn ESE370 Fall2016 – Khanna + + + - - - Vcap>0 42 MOS Field? ! What does “capacitor” field do to the Donor-doped semiconductor channel? Vgs=0 No field + - - - - - - = Penn ESE370 Fall2016 – Khanna + + + - - - +++++ Vcap>0 Vgs>0 Conducts -----43 MOS Field Effect ! Charge on capacitor " " " Attract or repel charges to form channel Modulates conduction Positive " " Attracts carriers " Enables conduction Negative? " Repel carriers " Disable conduction +++++ ----------- Penn ESE370 Fall2016 – Khanna 44 Doping ! What happens if we replace Si atoms with group 13 atom instead? " " E.g. B (Boron) Valance band electrons? B Penn ESE370 Fall2016 – Khanna 45 Doping with B ! End up with electron vacancies -- Holes " ! Acceptor electron sites Easy for electrons to shift into these sites " " Low energy to displace Easy for the electrons to move " Movement of an electron best viewed as movement of hole Penn ESE370 Fall2016 – Khanna 46 Doped Band Gaps ! Addition of acceptor sites makes more metallic " Easier to conduct Semiconductor Ec 0.045ev 1.1ev Penn ESE370 Fall2016 – Khanna EA Ev 47 Hole Conduction Penn ESE370 Fall2016 – Khanna 48 Field Effect? ! Effect of positive field on Acceptor-doped Silicon? Vgs=0 No field + + + + Penn ESE370 Fall2016 – Khanna 49 Field Effect? ! Effect of positive field on Acceptor-doped Silicon? Vgs=0 No field + + + + + Penn ESE370 Fall2016 – Khanna + + + - - - Vcap>0 50 Field Effect? ! Effect of positive field on Acceptor-doped Silicon? Vgs=0 No field + + + + + = Penn ESE370 Fall2016 – Khanna + + + - - - +++++ Vcap>0 Vgs>0 No conduction 51 Field Effect? ! Effect of negative field on Acceptor-doped Silicon? Vgs=0 No field + + + + + Penn ESE370 Fall2016 – Khanna - - + + + Vcap<0 52 Field Effect? ! Effect of negative field on Acceptor-doped Silicon? Vgs=0 No field + + + + + + + + - - - = Penn ESE370 Fall2016 – Khanna - - Vcap<0 Vgs>0 Conduction +++++ 53 MOSFETs ! Donor doping " " " ! Excess electrons Negative or N-type material NFET Acceptor doping " " " Excess holes Positive or P-type material PFET Penn ESE370 Fall2016 – Khanna 54 Big Ideas: MOSFET ! ! Semiconductor can act like metal or insulator Use electric field to modulate conduction state of semiconductor -----+++++ Penn ESE370 Fall2016 – Khanna 55 Admin ! HW due Wednesday Penn ESE370 Fall2016 – Khanna 56